The FBD model [1]} in its extended
version[2]} serves to calculate cross sections for the synthesis of superheavy nuclei.
The extension consists in including the angular momentum dependence of all probabilities of successive stages in Eq. REF .
In other words, for each angular momentum (\(l\) ) the partial evaporation residue
cross section \(\sigma _{ER}(l)\)  for production of a given final nucleus in its ground state is factorized as the product of
the partial capture cross sections:
\(\sigma _{ER}(l) = ^{2} \pi \sum _{l=0}^{\infty } (2l+1) P_{cap}(l) P_{fus}(l) P_{sur}(l),\) 
